Net movement of electric charge through a medium– current ◦ Actually measures rate of charges passing through a cross-sectional area ◦ I = ΔQ/Δt SI Unit: Ampere (A) ◦ 1 A = 1 C/s Conventional current defined in terms of positive charge movement ◦ Actual motion of charges can be positive, negative or mixture of both ◦ Positive and negative charges in motion: charge carriers ◦ Conventional current defined as current consisting of positive charges that would have the same effect as the actual motion of the charge carriers, regardless of the actual charge of the charge carriers Charges set in motion by electric fields ◦ Good conductors permit easy motion of charge carriers Metals Electrolyte solutions Charge carriers move fairly slowly through media ◦ When switch is closed, electric field established through circuit ◦ Field sets charges in motion throughout wires ◦ Field moves at speed of light, charges move more slowly Drift velocity is net velocity of charge carriers ◦ In electrostatic equilibrium, charges move randomly ◦ A potential difference applied through wire generates electric field ◦ Forces sets charges in motion opposite electric field and establishes current Charges do not move in straight lines ◦ Matter of conductor blocks straight path ◦ Charges and vibrating particles create zigzag pattern in conductor ◦ Energy from charges transferred to conductor through collisions and increases their kinetic energy Conductor’s temperature rises Energy gained by charges as accelerated through electric field greater than loss due to collisions ◦ See net motion in direction opposite the electric field ◦ Velocity: drift velocity (vdrift) A potential difference applied to a conductor sets charges in motion from higher electric potential to lower electric potential ◦ Potential difference maintains current Batteries/generators maintain potential difference across terminals through conversions of energy ◦ Batteries: chemical to electrical ◦ Generators: mechanical to electrical Current may be direct or alternating ◦ Direct: charges move in only one direction ◦ Alternating: movement of charges continuously changes direction Batteries: each terminal has fixed sign so charge flows only one direction ◦ Direct current AC sources: terminals change sign constantly, so net flow of charge is 0 ◦ Slow motions can be seen with flickering of lights ◦ In US, AC operates at frequency of 60 Hz Opposition to the motion of a charge through a conductor Ratio of potential difference to current ◦ R = ΔV/I SI unit: ohm (Ω) For many materials, resistance is constant over wide range of potential differences ◦ ◦ ◦ ◦ Ohmic substances Ohm’s Law = ΔV/I = constant Δ = IR Graph of I vs V would be linear Non-ohmic substances: resistance not constant over voltage range ◦ Graph of I vs V would be nonlinear ◦ Diodes are non-ohmic Ohm’s Law not considered a fundamental law of nature Length, cross-sectional area, material, temperature Length: ↑Length, ↑Resistance X-section area: ↑Area, ↓Resistance Material: Electrical conductivity determines resistance Temperature: ↑Temperature, ↑Resistance Circuit components that regulate current flow ◦ May be a device (load) or component specificallydesigned to be resistor ◦ Usually cheaper to manipulate resistance than potential difference for electronic devices Materials that have zero resistance below a certain temperature ◦ Critical temperature ◦ Normal resistance pattern for most temperatures When temperature is at or below critical temperature, resistance suddenly drops to zero Thousands of substances are superconductors ◦ Aluminum, tin, zinc, lead Conductivity not an indicator of superconductivity ◦ Gold, silver, copper When current established in superconductor, current continues even when potential difference is removed ◦ May persist without decay for years ◦ Electric currents produce magnetic effects Meissner effect: interaction between a superconductor and a magnet causes magnet to levitate above superconductor Current research seeks superconductors at room temperatures ◦ Superconductivity found in some substances up to 150K ◦ Energy requirements for cooling materials to very low temperatures is high Benefits from superconductivity often outweighed by costs As charges move through a system, they lose energy due to collisions with other particles and charge carriers ◦ Reach power source with zero potential energy ◦ Source must do work on charge to increase its potential Potential increases by QΔV Power source loses equivalent amount of energy Electric power is the rate of conversion of electric energy ◦ Rate at which charge carriers do work Power is the rate at which charge carriers convert electrical potential energy to nonelectrical forms of energy Formula: P = IΔV ◦ Describes rate at which charge carriers lose electrical potential energy SI Unit: Watt (W) Power dissipated by a resistor or load: ◦ P = I2R; P = (ΔV)2/R ◦ Joule heating: conversion of electrical energy to internal energy in resistant material Power lines subject to joule heating or I2R loss Power companies want to minimize loss and maximize energy delivered to consumer ◦ Can either decrease current or resistance ◦ Equation I2R states reducing current has more impact on joule heating than reducing resistance From P = IΔV, power can be delivered through high current/low voltage or high voltage/low current Power companies deliver electrical energy at very high voltages ◦ Transformers reduce voltages until power reaches homes at about 120V